Three-Dimensional Majorana Fermions in Chiral Superconductors
arXiv:1607.08243 · doi:10.1126/sciadv.1601835
Abstract
Through a systematic symmetry and topology analysis we establish that three-dimensional chiral superconductors with strong spin-orbit coupling and odd-parity pairing generically host low-energy nodal quasiparticles that are spin-non-degenerate and realize Majorana fermions in three dimensions. By examining all types of chiral Cooper pairs with total angular momentum formed by Bloch electrons with angular momentum in crystals, we obtain a comprehensive classification of gapless Majorana quasiparticles in terms of energy-momentum relation and location on the Fermi surface. We show that the existence of bulk Majorana fermions in the vicinity of spin-selective point nodes is rooted in the non-unitary nature of chiral pairing in spin-orbit-coupled superconductors. We address experimental signatures of Majorana fermions, and find that the nuclear magnetic resonance (NMR) spin relaxation rate is significantly suppressed for nuclear spins polarized along the nodal direction as a consequence of the spin-selective Majorana nature of nodal quasiparticles. Furthermore, Majorana nodes in the bulk have nontrivial topology and imply the presence of Majorana bound states on the surface that form arcs in momentum space. We conclude by proposing the heavy fermion superconductor PrOsSb and related materials as promising candidates for non-unitary chiral superconductors hosting three-dimensional Majorana fermions.
12 pages, 3 figures + appendices; published version
References in corpus (21)
- Topological Photonics
- The Order Parameter for the Superconducting Phases of UPt
- Chiral P-Wave Order in Sr_2RuO_4
- Superconductivity of doped Weyl semimetals: finite-momentum pairing and electronic analogues of the 3He-A phase
- Nodal Structure of Unconventional Superconductors Probed by the Angle Resolved Thermal Transport Measurements
- Anomalous Andreev bound state in non-centrosymmetric superconductors
- Friedel oscillations due to Fermi arcs in Weyl semimetals
- Surface density of states and topological edge states in non-centrosymmetric superconductors
- Majorana Fermions in Nodal Superconductors: Gapless Topological Phase
- Superconductivity in the New Platinum Germanides MPt4Ge12 (M = Rare-earth and Alkaline-earth Metals) with Filled Skutterudite Structure
- Nodal Structure of Superconductors with Time-Reversal Invariance and Z2 Topological Number
- Topologically protected flat zero-energy surface bands in non-centrosymmetric superconductors
- Crossed surface flat bands of Weyl semimetal superconductors
- Relativistic analysis of the pairing symmetry of the noncentrosymmetric superconductor LaNiC
- Majorana surface states of superfluid 3He A- and B-phases in a slab
- Exotic multi-gap structure in UPt unveiled by the first-priniciples analysis
- Superconducting states in the tetrahedral compound PrOs4Sb12
- Topological Fermi arcs in superfluid He
- Multiband superconductivity in PrPt4Ge12 single crystals
- Probing the superconductivity of PrPt4Ge12 through Ce substitution
- Surface Majorana fermions and bulk collective modes in superfluid 3He-B
Cited by in corpus (12)
- Complete classification of band nodal structures
- Nematic and chiral superconductivity induced by odd-parity fluctuations
- Topology and symmetry of surface Majorana arcs in cyclic superconductors
- Broken Time Reversal Symmetry in Superconducting Pr1-xCexPt4Ge12
- Broken time-reversal symmetry in superconducting PrLaPtGe
- Odd-Parity Quasiparticle Interference in the Superconductive Surface State of UTe2
- Topological Anomalous Skin Effect in Weyl Superconductors
- Spontaneous vortex-antivortex lattice and Majorana fermions in rhombohedral graphene
- Higher-order topological phases for time-reversal-symmetry breaking superconductivity in UTe
- Nuclear spin relaxation rate of nonunitary Dirac and Weyl superconductors
- Visualizing the Odd-parity Superconducting Order Parameter and its Quasiparticle Surface Band in UTe2
- Pairing-induced Momentum-space Magnetism and Its Implication In Optical Anomalous Hall Effect In Chiral Superconductors